Study of dipion bottomonium transitions and search for the h(b)(1P) state RID C-5223-2009
- Lees JP
- Poireau V
- Tisserand V
- Tico JG
- Grauges E
- Martinelli M
- Milanes DA
- Palano A
- Pappagallo M
- Eigen G
- Stugu B
- Sun L
- Brown DN
- Kerth LT
- Kolomensky YG
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- Koch H
- Schroeder T
- Asgeirsson DJ
- Hearty C
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- McKenna JA
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- Blinov VE
- Buzykaev AR
- Druzhinin VP
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- Kravchenko EA
- Onuchin AP
- Serednyakov SI
- Skovpen YI
- Solodov EP
- Todyshev KY
- Yushkov AN
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- Mandelkern M
- Stoker DP
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- Gary JW
- Liu F
- Long O
- Vitug GM
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- Richman JD
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- Lockman WS
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- Cheng CH
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- Dubrovin MS
- Meadows BT
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- Bloom PC
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- Monge MR
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- Edwards AJ
- Adametz A
- Marks J
- Uwer U
- Bernlochner FU
- Ebert M
- Lacker HM
- Lueck T
- Dauncey PD
- Tibbetts M
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- Mallik U
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- Crawley HB
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- Albert J
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- Nugent IM
- Roney JM
- Sobie RJ
- Gershon TJ
- Harrison PF
- Latham TE
- Puccio EMT
- Band HR
- Dasu S
- Pan Y
- Prepost R
- Vuosalo CO
- Wu SL
- LUSIANI, Alberto
Publication date
January 2011
DOIAbstract
We study inclusive dipion decays using a sample of 108 x 10(6)Y(3S) events recorded with the BABAR detector. We search for the decay mode Y(3S) -> pi(+)pi(-) h(b)(1P) and find no evidence for the bottomonium spin-singlet state h(b)(1P) in the invariant mass distribution recoiling against the pi(+)pi(-) system. Assuming the h(b)(1P) mass to be 9.900 GeV/c(2), we measure the upper limit on the branching fraction B[Y(3S) -> pi(+)pi(-) h(b)(1P)] pi(+)pi(-) chi(bJ)(1P), Y(3S) -> pi(+)pi(-) Y(2S), and Y(2S) -> pi(+)pi(-) Y(1) dipion transitions and present an improved measurement of the branching fraction of the Y(3S) -> pi(+)pi(-) Y(2S) decay and of the Y(3S) - Y(2S) mass difference
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